CURRENT EXPERIMENTS in PARTICLE PHYSICS Particle Data Group
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CERN Courier–Digital Edition
CERNMarch/April 2021 cerncourier.com COURIERReporting on international high-energy physics WELCOME CERN Courier – digital edition Welcome to the digital edition of the March/April 2021 issue of CERN Courier. Hadron colliders have contributed to a golden era of discovery in high-energy physics, hosting experiments that have enabled physicists to unearth the cornerstones of the Standard Model. This success story began 50 years ago with CERN’s Intersecting Storage Rings (featured on the cover of this issue) and culminated in the Large Hadron Collider (p38) – which has spawned thousands of papers in its first 10 years of operations alone (p47). It also bodes well for a potential future circular collider at CERN operating at a centre-of-mass energy of at least 100 TeV, a feasibility study for which is now in full swing. Even hadron colliders have their limits, however. To explore possible new physics at the highest energy scales, physicists are mounting a series of experiments to search for very weakly interacting “slim” particles that arise from extensions in the Standard Model (p25). Also celebrating a golden anniversary this year is the Institute for Nuclear Research in Moscow (p33), while, elsewhere in this issue: quantum sensors HADRON COLLIDERS target gravitational waves (p10); X-rays go behind the scenes of supernova 50 years of discovery 1987A (p12); a high-performance computing collaboration forms to handle the big-physics data onslaught (p22); Steven Weinberg talks about his latest work (p51); and much more. To sign up to the new-issue alert, please visit: http://comms.iop.org/k/iop/cerncourier To subscribe to the magazine, please visit: https://cerncourier.com/p/about-cern-courier EDITOR: MATTHEW CHALMERS, CERN DIGITAL EDITION CREATED BY IOP PUBLISHING ATLAS spots rare Higgs decay Weinberg on effective field theory Hunting for WISPs CCMarApr21_Cover_v1.indd 1 12/02/2021 09:24 CERNCOURIER www. -
Arxiv:2010.09509V2 [Hep-Ph] 2 Apr 2021 in Searches for CLFV Or LNV, Incoming Muons Are the Source of Both the Μ → E Signal and the RMC Back- Ground
FERMILAB-PUB-20-525-T The high energy spectrum of internal positrons from radiative muon capture on nuclei Ryan Plestid1, 2, ∗ and Richard J. Hill1, 2, y 1Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40506, USA 2Theoretical Physics Department, Fermilab, Batavia, IL 60510,USA (Dated: April 5, 2021) The Mu2e and COMET collaborations will search for nucleus-catalyzed muon conversion to positrons (µ− ! e+) as a signal of lepton number violation. A key background for this search is radiative muon capture where either: 1) a real photon converts to an e+e− pair “externally" in surrounding material; or 2) a virtual photon mediates the production of an e+e− pair “internally”. If the e+ has an energy approaching the signal region then it can serve as an irreducible background. In this work we describe how the near end-point internal positron spectrum can be related to the real photon spectrum from the same nucleus, which encodes all non-trivial nuclear physics. I. INTRODUCTION Specifically, on a nucleus (e.g. aluminum), the reaction µ− + [A; Z] ! e+ + [A; Z − 2] ; (1) Charged lepton flavor violation (CLFV) is a smok- ing gun signature of physics beyond the Standard Model becomes a viable target for observation (see also [7]). (SM) and is one of the most sought-after signals at the While neutrinoless double beta (0νββ) decay is often intensity frontier [1–4]. Important search channels in- touted as the most promising direction for the discovery volving the lightest two lepton generations are µ ! 3e, of LNV, there do exist extensions of the SM that predict µ ! eγ, and nucleus-catalyzed µ ! e [1–6]. -
Subnuclear Physics: Past, Present and Future
Subnuclear Physics: Past, Present and Future International Symposium 30 October - 2 November 2011 – The purpose of the Symposium is to discuss the origin, the status and the future of the new frontier of Physics, the Subnuclear World, whose first two hints were discovered in the middle of the last century: the so-called “Strange Particles” and the “Resonance #++”. It took more than two decades to understand the real meaning of these two great discoveries: the existence of the Subnuclear World with regularities, spontaneously plus directly broken Symmetries, and totally unexpected phenomena including the existence of a new fundamental force of Nature, called Quantum ChromoDynamics. In order to reach this new frontier of our knowledge, new Laboratories were established all over the world, in Europe, in USA and in the former Soviet Union, with thousands of physicists, engineers and specialists in the most advanced technologies, engaged in the implementation of new experiments of ever increasing complexity. At present the most advanced Laboratory in the world is CERN where experiments are being performed with the Large Hadron Collider (LHC), the most powerful collider in the world, which is able to reach the highest energies possible in this satellite of the Sun, called Earth. Understanding the laws governing the Space-time intervals in the range of 10-17 cm and 10-23 sec will allow our form of living matter endowed with Reason to open new horizons in our knowledge. Antonino Zichichi Participants Prof. Werner Arber H.E. Msgr. Marcelo Sánchez Sorondo Prof. Guido Altarelli Prof. Ignatios Antoniadis Prof. Robert Aymar Prof. Rinaldo Baldini Ferroli Prof. -
Jul/Aug 2013
I NTERNATIONAL J OURNAL OF H IGH -E NERGY P HYSICS CERNCOURIER WELCOME V OLUME 5 3 N UMBER 6 J ULY /A UGUST 2 0 1 3 CERN Courier – digital edition Welcome to the digital edition of the July/August 2013 issue of CERN Courier. This “double issue” provides plenty to read during what is for many people the holiday season. The feature articles illustrate well the breadth of modern IceCube brings particle physics – from the Standard Model, which is still being tested in the analysis of data from Fermilab’s Tevatron, to the tantalizing hints of news from the deep extraterrestrial neutrinos from the IceCube Observatory at the South Pole. A connection of a different kind between space and particle physics emerges in the interview with the astronaut who started his postgraduate life at CERN, while connections between particle physics and everyday life come into focus in the application of particle detectors to the diagnosis of breast cancer. And if this is not enough, take a look at Summer Bookshelf, with its selection of suggestions for more relaxed reading. To sign up to the new issue alert, please visit: http://cerncourier.com/cws/sign-up. To subscribe to the magazine, the e-mail new-issue alert, please visit: http://cerncourier.com/cws/how-to-subscribe. ISOLDE OUTREACH TEVATRON From new magic LHC tourist trail to the rarest of gets off to a LEGACY EDITOR: CHRISTINE SUTTON, CERN elements great start Results continue DIGITAL EDITION CREATED BY JESSE KARJALAINEN/IOP PUBLISHING, UK p6 p43 to excite p17 CERNCOURIER www. -
CURRICULUM VITAE – Paul D. Grannis April 6, 2021 DATE of BIRTH: June 26, 1938 EDUCATION
CURRICULUM VITAE { Paul D. Grannis July 15, 2021 EDUCATION: B. Eng. Phys., with Distinction, Cornell University (1961) Ph.D. University of California, Berkeley (1965) Thesis: Measurement of the Polarization Parameter in Proton-Proton Scattering from 1.7 to 6.1 BeV Advisor, Owen Chamberlain EMPLOYMENT: Research Professor of Physics, State Univ. of New York at Stony Brook, 2007 { Distinguished Professor Emeritus, State Univ. of New York at Stony Brook, 2007 { Chair, Department of Physics and Astronomy, Stony Brook, 2002 { 2005 Distinguished Professor of Physics, State Univ. of New York at Stony Brook, 1997 { 2006 Professor of Physics, Stony Brook, 1975 { 1997 Associate Professor of Physics, Stony Brook, 1969 { 1975 Assistant Professor of Physics, Stony Brook, 1966 { 1969 Research Associate, Lawrence Radiation Laboratory, 1965 { 1966 1 AWARDS: Danforth Foundation Fellow, 1961 { 1965 Alfred P. Sloan Foundation Fellow, 1969 { 1971 Fellow, American Physical Society Fellow, American Association for the Advancement of Science Exceptional Teaching Award, Stony Brook, 1992 Exceptional Service Award, U.S. Department of Energy, 1997 John S. Guggenheim Fellowship, 2000 { 2001 American Physical Society W.K.H. Panofsky Prize, 2001 Honorary Doctor of Science, Ohio University, 2009 W. V. Houston Memorial Lectureship, Rice University 2012 Foreign member, Russian Academy of Science, 2016 Co-winner with the members of the DØ Collaboration, European Physical Society High Energy Particle Physics Prize, 2019 2 OTHER ACTIVITIES: Visiting Scientist, Rutherford -
Cusp Effects in Meson Decays
EPJ Web of Conferences 3, 01008 (2010) DOI:10.1051/epjconf/20100301008 © Owned by the authors, published by EDP Sciences, 2010 Cusp effects in meson decays Bastian Kubis,a Helmholtz-Institut f¨ur Strahlen- und Kernphysik (Theorie) and Bethe Center for Theoretical Physics, Universit¨at Bonn, D-53115 Bonn, Germany Abstract. The pion mass difference generates a pronounced cusp in the π0π0 invariant mass distribution of K+ π0π0π+ decays. As originally pointed out by Cabibbo, an accurate measurement of the cusp may allow one to pin→ down the S-wave pion–pion scattering lengths to high precision. We present the non-relativistic effective field theory framework that permits to determine the structure of this cusp in a straightforward manner, including the effects of radiative corrections. Applications of the same formalism to other decay channels, in particular η and η′ decays, are also discussed. 1 The pion mass and pion–pion scattering alternative scenario of chiral symmetry breaking under the name of generalized chiral perturbation theory [4]. The approximate chiral symmetry of the strong interac- Fortunately, chiral low-energy constants tend to appear tions severely constrains the properties and interactions in more than one observable,and indeed, ℓ¯3 also features in of the lightest hadronic degrees of freedom, the would-be the next-to-leading-order corrections to the isospin I = 0 0 Goldstone bosons (in the chiral limit of vanishing quark S-wave pion–pion scattering length a0 [2], masses) of spontaneous chiral symmetry breaking that can be identified with the pions. The effective field theory that 7M2 0 = π + ǫ + 4 , a0 2 1 (Mπ) systematically exploits all the consequencesthat can be de- 32πFπ O rived from symmetries is chiral perturbation theory [1,2], 5M2 n 3 o 21 21 which provides an expansion of low-energy observables in = π ¯ + ¯ ¯ + ¯ + ǫ 2 2 ℓ1 2ℓ2 ℓ3 ℓ4 . -
Kenneth A. Merique Genealogical and Historical Collection BOOK NO
Kenneth A. Merique Genealogical and Historical Collection SUBJECT OR SUB-HEADING OF SOURCE OF BOOK NO. DATE TITLE OF DOCUMENT DOCUMENT DOCUMENT BG no date Merique Family Documents Prayer Cards, Poem by Christopher Merique Ken Merique Family BG 10-Jan-1981 Polish Genealogical Society sets Jan 17 program Genealogical Reflections Lark Lemanski Merique Polish Daily News BG 15-Jan-1981 Merique speaks on genealogy Jan 17 2pm Explorers Room Detroit Public Library Grosse Pointe News BG 12-Feb-1981 How One Man Traced His Ancestry Kenneth Merique's mission for 23 years NE Detroiter HW Herald BG 16-Apr-1982 One the Macomb Scene Polish Queen Miss Polish Festival 1982 contest Macomb Daily BG no date Publications on Parental Responsibilities of Raising Children Responsibilities of a Sunday School E.T.T.A. BG 1976 1981 General Outline of the New Testament Rulers of Palestine during Jesus Life, Times Acts Moody Bible Inst. Chicago BG 15-29 May 1982 In Memory of Assumption Grotto Church 150th Anniversary Pilgrimage to Italy Joannes Paulus PP II BG Spring 1985 Edmund Szoka Memorial Card unknown BG no date Copy of Genesis 3.21 - 4.6 Adam Eve Cain Abel Holy Bible BG no date Copy of Genesis 4.7- 4.25 First Civilization Holy Bible BG no date Copy of Genesis 4.26 - 5.30 Family of Seth Holy Bible BG no date Copy of Genesis 5.31 - 6.14 Flood Cainites Sethites antediluvian civilization Holy Bible BG no date Copy of Genesis 9.8 - 10.2 Noah, Shem, Ham, Japheth, Ham father of Canaan Holy Bible BG no date Copy of Genesis 10.3 - 11.3 Sons of Gomer, Sons of Javan, Sons -
The Discovery of the Higgs Boson at the LHC
Chapter 6 The Discovery of the Higgs Boson at the LHC Peter Jenni and Tejinder S. Virdee 6.1 Introduction and the Standard Model The standard model of particle physics (SM) is a theory that is based upon principles of great beauty and simplicity. The theory comprises the building blocks of visible matter, the fundamental fermions: quarks and leptons, and the fundamental bosons that mediate three of the four fundamental interactions; photons for electromag- netism, the W and Z bosons for the weak interaction and gluons for the strong interaction (Fig. 6.1). The SM provides a very successful description of the visible universe and has been verified in many experiments to a very high precision. It has an enormous range of applicability and validity. So far no significant deviations have been observed experimentally. The possibility of installing a proton-proton accelerator in the LEP tunnel, after the e+e− programme, was being discussed in the 1980’s. At the time there were many profound open questions in particle physics, and several are still present. In simple terms these are: what is the origin of mass i.e. how do fundamental particles acquire mass, and why do they have the masses that they have? Why is there more matter than anti-matter? What is dark matter? What is the path towards unification of all forces? Do we live in a world with more space-time dimensions than the familiar four? The LHC [1, 2] was conceived to address or shed light on these questions. P. Jenni CERN, Geneva, Switzerland Albert-Ludwigs University Freiburg, Freiburg im Breisgau, Germany T. -
4 Muon Capture on the Deuteron 7 4.1 Theoretical Framework
February 8, 2008 Muon Capture on the Deuteron The MuSun Experiment MuSun Collaboration model-independent connection via EFT http://www.npl.uiuc.edu/exp/musun V.A. Andreeva, R.M. Careye, V.A. Ganzhaa, A. Gardestigh, T. Gorringed, F.E. Grayg, D.W. Hertzogb, M. Hildebrandtc, P. Kammelb, B. Kiburgb, S. Knaackb, P.A. Kravtsova, A.G. Krivshicha, K. Kuboderah, B. Laussc, M. Levchenkoa, K.R. Lynche, E.M. Maeva, O.E. Maeva, F. Mulhauserb, F. Myhrerh, C. Petitjeanc, G.E. Petrova, R. Prieelsf , G.N. Schapkina, G.G. Semenchuka, M.A. Sorokaa, V. Tishchenkod, A.A. Vasilyeva, A.A. Vorobyova, M.E. Vznuzdaeva, P. Winterb aPetersburg Nuclear Physics Institute, Gatchina 188350, Russia bUniversity of Illinois at Urbana-Champaign, Urbana, IL 61801, USA cPaul Scherrer Institute, CH-5232 Villigen PSI, Switzerland dUniversity of Kentucky, Lexington, KY 40506, USA eBoston University, Boston, MA 02215, USA f Universit´eCatholique de Louvain, B-1348 Louvain-la-Neuve, Belgium gRegis University, Denver, CO 80221, USA hUniversity of South Carolina, Columbia, SC 29208, USA Co-spokespersons underlined. 1 Abstract: We propose to measure the rate Λd for muon capture on the deuteron to better than 1.5% precision. This process is the simplest weak interaction process on a nucleus that can both be calculated and measured to a high degree of precision. The measurement will provide a benchmark result, far more precise than any current experimental information on weak interaction processes in the two-nucleon system. Moreover, it can impact our understanding of fundamental reactions of astrophysical interest, like solar pp fusion and the ν + d reactions observed by the Sudbury Neutrino Observatory. -
Status of the Alcap Experiment
Status of the AlCap experiment R. Phillip Litchfield∗† UCL E-mail: [email protected] The AlCap experiment is a joint project between the COMET and Mu2e collaborations. Both experiments intend to look for the lepton-flavour violating conversion m + A ! e + A, using ter- tiary muons from high-power pulsed proton beams. In these experiments the products of ordinary muon capture in the muon stopping target are an important concern, both in terms of hit rates in tracking detectors and radiation damage to equipment. The goal of the AlCap experiment is to provide precision measurements of the products of nuclear capture on Aluminium, which is the favoured target material for both COMET and Mu2e. The results will be used for optimising the design of both conversion experiments, and as input to their simulations. Data was taken in December 2013 and is currently being analysed. 16th International Workshop on Neutrino Factories and Future Neutrino Beam Facilities - NUFACT2014, arXiv:1501.04880v1 [physics.ins-det] 20 Jan 2015 25 -30 August, 2014 University of Glasgow, United Kingdom ∗Speaker. †On behalf of the AlCap Collaboration © Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it/ Status of the AlCap experiment R. Phillip Litchfield 1. Muon to electron conversion and the motivation for AlCap The term ‘muon to electron conversion’ refers to processes that cause the neutrinoless decay of a muon into an electron, specifically those in which the muon is the ground-state orbit of an atomic nucleus.1 In this case the conservation of momentum and energy can be achieved by coherent interaction on the nucleus, i.e. -
Kent County Naturalization Name Index, Aalbers, A
Kent County Naturalization Name Index Last name First name Middle name Volume Page Fir Sec Aalbers Aalbers V62 4 Aalbers Aalbert V24 141 Aalddriks Antonie V16 75 Aalderink John K. V16 355 Aaldrick Matthew V16 308 Aardem Arie V16 304 Aardema Klaas V17 27 Aarnouds Pieter V6 8 Aarnoudse Marenus V15 503 Abagis Chas V30 130 Abbas Sain Allez V49 265 Abbelma Joseph B1 F5 Abbelma Joseph V2 564 Abbott Frank V27 92 Abbott John V45 36 Abbott John V68 33 Abdella Salik V46 117 Abdo Ahamad V29 1 Abdoo Mike V41 168 Abeaf Moses V17 391 Abeaf Moses V17 394 Abel Frederick FW B1 F1 Abel Gustav B1 F4 Abel Gustav V2 540 Abel John W. V5 70 Abel Ludwig V8 134 Friday, January 19, 2001 Page 1 of 1325 Last name First name Middle name Volume Page Fir Sec Abella Salih V68 85 Abezi Albert V25 76 Aboabsee Theab V74 40 Aboasee Theab V18 150 Abood N. B1 F5 Abood Nemy V3 90 Abraham John V17 381 Abrahamson Charles Y. B7 200 Abram John B1 F1 Abramson Morris B1 F3 Abraursz Abram Peter V27 159 Abromaitis Louis V27 381 Abromaitis Louis V67 90 Absmaier Carl V77 4 Accardi Guiseppe V50 79 Acheson John V16 616 Achille Minciotti V51 142 Achtenhof Jakob V15 145 Achter Jan V17 200 Achterhof Henri B1 F1 Achterhof Johannes V15 500 Achterhof Matheus B1 F1 Achtjes John B7 107 Ackermann Joseph V15 282 Acton John C. B7 222 Adair David G. V15 335 Adair Joseph V15 335 Adalphson Emil V18 197 Friday, January 19, 2001 Page 2 of 1325 Last name First name Middle name Volume Page Fir Sec Adam Frickartz Heinrich V41 279 Adama Jelle V22 176 Adamawiczus Baltris V37 155 Adamczak Peter V38 245 Adamczyk Wladyslaw V35 291 Adams Edward John V24 70 Adams Frank B1 F2 Adams George W. -
Wayne County Death Index, 1934-1939 1 SURNAME FIRST
SURNAME FIRST NAME MIDDLE AGE DATE LOCATION BOX FILE Aaron Phillip W 305 4/21/1938 WD 21 16 Aarons Victoria 149 10/9/1937 EC 13 16 Abbeg Minnie Manning 160 7/13/1938 SM TP 21 8 Abbey Thomas J 180 8/7/1939 HP 30 16 Abbote Vito 165 3/3/1938 NK TP 23 7 Abbott Ada 180 3/2/1938 HP 22 3 Abbott Blanche Maude 152 5/24/1938 HP 22 7 Abbott Chester 155 10/21/1938 WD 21 20 Abbott Ira W 190 8/20/1935 WY 6 11 Abbott Melvin J 102 3/31/1936 WD 9 15 Abbott Roy 142 6/24/1937 WD 15 19 Abbott William C 184 9/28/1936 RM TP 8 14 Abell Ellen 163 2/20/1937 NK TP 17 8 Abelson James H 183 11/27/1938 NK TP 24 12 Aben Augusta 171 11/25/1937 LP 14 15 Abernathy Paul 152 4/3/1939 NK TP 28 16 Abjorson Sven J 148 8/2/1938 GPF 19 16 Abraham Anna 155 4/3/1938 HP 22 5 Abraham Fay 142 9/17/1939 WD 27 22 Abraham Frank Wilson 119 2/18/1937 HP 16 4 Abraham Omar 150 8/2/1938 NK TP 24 1 Abrahamson John 157 12/22/1937 NK TP 18 16 Abram William 175 11/3/1937 NK TP 18 12 Abshagen William 163 2/11/1937 NK TP 17 7 Acciaccafero Dora 159 5/21/1939 NK TP 28 23 Acker Baby 0 4/12/1936 ML 7 27 Acker William H 187 8/12/1939 HP 30 16 Ackerman Jessie W 165 5/31/1939 WD 27 18 Ackerman Leo 174 4/15/1935 NK TP 4 14 Ackermann Joseph M 167 4/15/1936 HP 10 7 Ackersville William 141 10/30/1935 HP 3 19 Ackley Robert D 106 6/28/1936 HP 10 12 Adach John 150 8/17/1939 NK TP 29 7 Adair Baby 0 8/28/1939 WD 27 21 Adair Kristine Ann 105 5/6/1937 WD 15 17 Adamczak Baby 0 7/8/1935 HM 1 29 Adamczak Veronika 301 1/14/1939 HM 31 1 Adamczyk Baby 0 8/3/1937 HM 14 8 Adamczyk Donald 204 2/6/1937 HM 14 2 Adamczyk